|Publication number||US4464669 A|
|Application number||US 06/388,976|
|Publication date||Aug 7, 1984|
|Filing date||Jun 16, 1982|
|Priority date||Jun 19, 1981|
|Also published as||CA1187741A, CA1187741A1, DE3273429D1, EP0068702A2, EP0068702A3, EP0068702B1|
|Publication number||06388976, 388976, US 4464669 A, US 4464669A, US-A-4464669, US4464669 A, US4464669A|
|Inventors||Kunihiko Sekiya, Mamoru Mizuguchi, Takashi Ohzeki|
|Original Assignee||Tokyo Shibaura Denki Kabushiki Kaisha|
|Export Citation||BiBTeX, EndNote, RefMan|
|Patent Citations (10), Non-Patent Citations (1), Referenced by (56), Classifications (4), Legal Events (6)|
|External Links: USPTO, USPTO Assignment, Espacenet|
This invention is a thermal printer which is suitable for high speed printing with high quality.
Thermal printers have come into widespread use in various types of printers including those incorporated in facsimile equipment for recording picture images. Conventional thermal printers have a number of heating resistors arranged in a row on a substrate. These resistors are cyclically heated by selectively supplying electric current according to picture data. An image is recorded on a heat-sensitive paper which faces the heating resistors while the paper is moved in the direction perpendicular to the resistor array. While this kind of thermal printer is characterized by absence of noise, clean recording and ease of maintenance, a less desirable feature has been the difficulty of raising the speed of printing due to the heat-storage effect of the heating resistors. If, that is to say, the duty cycle is shortened in order to achieve high speed, heat is accumulated in the resistors since electrical current is repeatedly applied to the resistors before the heat generated in the previous cycle has been dissipated, so that the temperature continues to rise. Since the amount of heat accumulated in the resistors is different for each one depending on the picture data, this leads to a lack of uniformity in printing density. Further, the fact that the heat of the previous cycle remains up to the next cycle can lead to darkening of the heat-sensitive paper in places where there are space data, that is, where there should be no such darkening, so that ghost images appear.
In order to solve this problem, a method has been proposed whereby, for each heating resistor, if mark data arrive continuously in the picture signal data, the duty cycle (current passage time or pulse width) is made shorter than if mark data arrive after space data (Japan Patent Publication 55-48631). Realizing the principle, the method requires at least five gate circuits for each heating resistor which may number as many as 1000 to 2000. The thermal printer according to the prior art has, therefore, defects in that it is complicated, costly and not compact.
It is an object of the present invention to provide a thermal printer overcoming the disadvantages of the conventional printer by utilizing a simpler circuit.
It is a further object of the present invention to provide a thermal printer having a compact size.
It is a further object of the present invention to provide a thermal printer whereby high-speed printing can be attained while maintaining a high printing quality, especially for picture image printing.
According to the present invention, a plurality of resistors for generating heat are arranged in a line on a substrate. A power source supplies the heating resistors with electric power. The power source is connected to one end of each of the heating resistors via a drive circuit. The drive circuits are controlled by energy code signals which indicate the amount of electric energy to be supplied to each resistor from the power source. The energy codes for each heating resistor are stored in a memory which is written afresh for each printing cycle. The energy codes indicating the amounts of energy to be supplied to each heating resistor in the upcoming cycle of printing are determined by a logic circuit, based at least on (1) the energy codes which are stored in the memory and already used for printing in the previous cycle of printing, and (2) picture data to be printed in the upcoming cycle of printing. A second control circuit controls the timing of reading the enery codes from, and writing them into, the memory. The second control circuit also controls the timing of supplying the energy codes which have been read out from the memory.
FIG. 1 is a block diagram showing an embodiment of a thermal head incorporated in a thermal printer of the invention.
FIG. 2 is a block diagram showing an embodiment of the thermal printer according to the present invention.
FIG. 3 is a time chart illustrating the operation of the thermal printer of FIG. 2.
FIG. 4 is a block diagram showing a first control circuit connected to the thermal head of FIG. 1.
FIG. 5 is a time chart showing the operation of the first control circuit of FIG. 4.
FIG. 6 is a block diagram describing another embodiment of the thermal printer according to the present invention.
FIG. 7 symbolically illustrates the amounts of energy supplied to several heating resistors of the thermal head.
FIG. 8 is a time chart defining the symbols used in FIG. 7.
FIG. 9 is a time chart showing transmission times of facsimile picture data.
FIG. 10 is a graph of the relationship between printing cycle time and printing density in a thermal printer.
FIG. 11 is a block diagram showing a third embodiment of the thermal printer according to the present invention.
FIG. 12 is a block diagram of an embodiment of the transmission time detection circuit shown in FIG. 11.
FIG. 13 is a block diagram showing still another embodiment of the thermal printer according to the present invention.
FIG. 14 depicts a modification of the multiplexer shown in FIG. 4.
FIG. 15 is a time chart showing the operation of the thermal printer in the embodiment of FIG. 14.
FIG. 16 is a block diagram of a modification of the thermal printer shown in FIG. 6.
FIG. 17 is a block diagram of an alternate form of memory for the present invention.
FIG. 18 is a block diagram showing a modification of the thermal head of the invention.
FIG. 1 schematically shows a printing head incorporated in one embodiment of the invention. A plurality of heating resistors 121, 122, - - - 12n are arranged in a line on a substrate 14 made of a ceramic material. The number of resistors may be 1000 to 2000 or more. A plurality of drive circuits 161, 162, - - - 16n are provided on substrate 14, each drive circuit being connected in series with one of the heating resistors. A power source 18 such as a voltaic cell is connected to a pair of power terminals 201 and 202 between which are connected the sets of heating resistors and drive circuits. An n-bit shift register 22 is provided on substrate 14. Output terminals of each shift stage 241, 242, - - - 24n are connected to drive circuits 161, 162, - - - 16n to control the drive circuits. The drive circuits have a gate function for selectively supplying direct current from power source 18 to the resistors according to the gating signals from the shift register. Gating signals consisting of 1's and 0's (which respectively correspond to "mark" and "space" in the picture) are supplied to shift register 22 through an input terminal 26. Shift register 22 is driven by clock pulses CK supplied to it from a terminal 28.
The shift register also has a latch function. After a set of data to be printed is shifted into the register, a latch pulse is needed to cause drive circuits 16 to drive the heating resistor 12. The latch pulses are supplied through terminal 30. When the first latch pulse arrives, those drive circuits corresponding to stages of the shift register which hold a "1" are enabled to apply power to their heating resistors. The other drive circuits remain disabled. While power is being applied to the heating resistors, the next set of data is shifted into the shift register. When the next latch pulse arrives, drive circuits are enabled in accordance with this new data. The bits from the shift register are therefore "latched," or maintained, during the time between latch pulses.
When n bits of printing data have been moved serially into shift register 22 by clock pulses CK, all mark bits (1's) among output terminals 241, 242, - - - 24n selectively open the gates of the corresponding drive circuits 161, 162, - - - 16n. Electric current from power source 18 is supplied to the selected heating resistors to generate heat. The heated resistors print marks in a line along the resistor array on a heat sensitive paper (not shown) which faces the heating resistors while it is moved in a direction perpendicular to the resistor array. After one line of marks is printed, another set of printing data is supplied to shift register 22; and a similar printing cycle is repeated for printing each following line while the heat-sensitive paper is moving.
The amount of electric energy to be supplied to each of the resistors is determined by taking into consideration the amount which was supplied to each resistor during the previous printing cycle. FIG. 2 shows the whole system of a thermal printer according to the invention in which the amount of energy for each of n heating resitors is determined. Input information G in binary digital form are serially provided from a data input terminal 32 to an address decoder 34. Address decoder 34 also receives as input signals an energy code (M1, M2) from the previous printing cycle. The energy code (M1, M2) is a 2-digit binary code representing the amount of electrical energy which was supplied to a given heating resistor during the previous printing cycle. Address decoder 34 converts its input into 3-digit address codes (G, M1, M2) and supplies them to a read only memory 36 (hereinafter referred to as ROM). ROM 36 stores output codes (O1, O2) in addresses designated by the address codes (G, M1, M2). Output codes (O.sub. 1, O2) are also 2-digit binary codes representing electrical energy. A relationship (shown in Truth Table (1)) is established between the address codes (G, M1, M2) and the output codes (O1, O2) of ROM 36.
TRUTH TABLE (1)______________________________________G M1 M2 O1 O2______________________________________0 0 0 0 01 0 0 1 10 1 0 0 01 1 0 0 10 0 1 0 01 0 1 0 10 1 1 0 01 1 1 1 0______________________________________
Output codes (O1, O2) of ROM 36 are next stored in a random access memory 38 (hereinafter referred to as RAM) in addresses designated by address counter 40. As explained later, these output codes (O1, O2) are then read out from RAM 38 and supplied to a first control circuit 42 as an energy code (N1, N2) which should be printed in the subsequent printing cycle. Control circuit 42 controls the thermal head 44 by driving shift register 22 of FIG. 1 as explained later. A second control circuit 46 controls the operation of address decoder 34, ROM 36, RAM 38 and address counter 40.
Operation of the system shown in FIG. 2 is explained referring to the time chart of FIG. 3. RAM 38 is set to a read-out mode by write/read switching signal WR and a reset signal RES is supplied, at time t1, to address counter 40. The address counter designates by its output signal Qo, Q1, - - - Q9 the "0" address of RAM 38. The contents of the "0" address are read out at time t2 in response to a chip select signal CS2 (which selects RAM 38), and supplied to address decoder 34 as the energy code (M1, M2) of the previous cycle. Code (M1, M2) is latched by address decoder 34 together with a first bit G1 of incoming information signal G when a strobe signal STB is supplied from second control circuit 46. The address designation of ROM 36 is carried out by means of the output data of address decoder 34, and the content of this address is read out, at time t3, under the control of the chip select signal CS1 (which selects ROM 36) and a read-command signal RD. Output code (O1, O2) of ROM 36 is written into the "0" address of RAM 38, at time t4 in response to the chip select signal CS2 and the read/write switching signal WR which has set RAM 38 to the writing mode. At time t5, one clock signal CK is sent to address counter 40 designating the "1" address of RAM 38; and a similar operation is repeated for a second bit G2 of incoming information G. Thus, for further bits of input information G3, G4 - - -, Gn (not shown), the operations of reading RAM 38 and ROM 36 and of writing into RAM 38 are repeated n times. When the incoming information for one line, i.e., n bits (corresponding to the number of heating resistors) has been input, the amount of electrical energy to be supplied to each heating resistor for the first printing cycle is stored in RAM 38. In this case, as is clear from the Truth Table (1), codes (N1, N2 ) for the first cycle will be N1 =N2 =0 if G=0 or N1 =N2 =1 if G=1, since energy codes (M1, M2) are always 0 for the first printing cycle.
When the incoming information G of a second line is provided to input terminal 32, a similar operation is repeated; but in this case, since data indicating the amount of electric energy used in the first printing cycle have already been stored in RAM 38, output codes (O1, O2) of ROM 36 are obtained according to Truth Table (1); and these converted codes (O1, O2) are written afresh into RAM 38. Thereafter, exactly the same operation takes place when input occurs of data G of a third and subsequent lines.
Codes (N1, N2) indicating the amount of electrical energy in the coming cycle of printing are supplied to first control circuit 42 for controlling thermal head 44. FIG. 4 shows a block diagram of the first control circuit 42 together with the block diagram of thermal head 44 already shown in FIG. 1. First control circuit 42 comprises a decoder 422, a multiplexer 424 and a timing circuit 426. Decoder 422 converts energy data (N1, N2) supplied from RAM 38 in FIG. 2 into three-bit data words or pulse width codes (Q1, Q2, Q3) according to the following Truth Table (2).
TRUTH TABLE (2)______________________________________N1 N2 Q1 Q2 Q3______________________________________0 0 0 0 01 0 1 0 00 1 0 1 01 1 0 0 1______________________________________
Supplied with one of the pulse width codes (Q1, Q2, Q3), multiplexer 424 selectively outputs gating signals Y. The decision of what to output is carried out following Table (3) under the control of selection signals (S1, S2) supplied from timing control 426.
TABLE (3)______________________________________S1 S2 Y______________________________________0 0 *1 0 Q10 1 Q21 1 Q3______________________________________ *not used
The details of printing will now be explained according to time charts in FIG. 5. For each printing cycle (in which a single line of data is printed on heat sensitive paper), the same n sets of data (N1, N2) indicating the amount of electric energy for each of n heating resistors of the thermal printer are read out 3 times from RAM 38 as shown by I, II and III in FIG. 5. The numbers I, II and III indicate subcycle periods comprising a whole printing cycle for one line of printing data. During the first subcycle period n sets of data (N1, N2) stored in RAM 38 corresponding to one line of printing data are read out and converted into gating signals Y by decoder 422 and multiplexer 424. The first group of gating signals Y, that is corresponding to Q1, is supplied via input terminal 26 to shift register 22. The contents of shift register 22 are shifted in a bit by bit fashion by clock pulse CK from timing circuit 426. In this way all the first gating signals Y (corresponding to Q1) are input into shift register 22, a first latch pulse LP1 is supplied to shift register 22 from timing circuit 426 at the timing shown in FIG. 5. Latch pulse LP1 latches output signals of output terminals 241, 242, - - - 24n of the shift register for the period T1, until a second latch pulse LP2 is supplied as shown in FIG. 5. The output pulse signals T1 which take a value "1" or "0" corresponding to Q1 selectively drive circuits 161, 162, - - - 16n and electric current is supplied from power source 18 to the heating resistors during the period T1. The current is, however, supplied only to those resistors at which the mark data "1" of shift register 22 corresponds to the latched bit. In the second subcycle period, all the data (N1, N2) stored in RAM 38 are read out one by one and converted into pulse width codes (Q1, Q2, Q3) in turn. Since selection signals S1 and S2 are changed to "0" and "1" respectively by timing circuit 426, the second codes Q2 are selected as gating signals Y by multiplexer 424 and stored one by one into shift register 22. When all the signals Y are stored in shift register 22, the output signals of the register are latched by the second latch pulse LP2 for the period T2, which is longer than T1, until the third latch pulse LP3 is supplied as shown in FIG. 5. By this means, current is supplied to the selected heating resistors for the period T2. In the third subcycle period, all the data (N1, N2) are read out from RAM 38 and converted into pulse width codes (Q1, Q2, Q3). Since the selection signals S1 and S2 are both "1", the codes Q.sub. 3 selected by multiplexer 424. The current is supplied to the selected resistors for the period T3, which is longer than T2, by means of latching by the third latch pulse LP3 until the fourth latch pulse LP4 is supplied as shown in FIG. 5. One cycle of printing has, thus, been completed and another n sets of energy code (N1, N2) are processed in the same manner as mentioned above for the next line of printing. In this way, the same process is repeated for further lines of printing while the heat sensitive paper moves in a direction perpendicular to the lines of printing. It is understood from the Truth Tables (1)-(3) that the relationship between pulse width or current duration T(i-1) and T(i), in the (i-1)th and the i th lines of printing respectively, is shown in the following table in which pulse width or current duration T(i-1) and T(i) represent the amount of energy supplied to each heating resistor.
______________________________________ T(i - 1) T(i)______________________________________ 0 T3 T1 T2 T2 T2 T3 T1______________________________________
It can be seen from the table that T(i) is increased when T(i-1) is short and T(i) is decreased when T(i-1) is long; whereby uniformity in printing density can be obtained.
FIG. 6 shows another embodiment of the thermal printer in which the amount of energy to be supplied to each heating resistor in the subsequent cycle of printing is determined not only by the amount of energy supplied to that resistor during the previous printing cycle but also by the amount of energy supplied to adjacent resistors during the previous cycle. In a thermal printer for high density printing the heating resistors are also arranged with high density, i.e., 6 per mm or 8 per mm; so when current is actually passed through them, the temperature of each resistor is influenced by heat emitted from those nearby, particularly those next to it. This embodiment has been devised with this point in mind. In FIG. 6, a demultiplexer 62 is added to the block diagram shown in FIG. 2. Energy codes (M1, M2) are read out from RAM 38 and supplied to demultiplexer 62. In this embodiment, not only the energy code for each heating resistor in the previous cycle of printing but also two energy codes for the two adjacent resistors are read out from RAM 38 one by one and distributed to the output terminals A1, A2, B1, B2, C1, C2 of demultiplexer 62. Output terminals (B1, B2) are supplied with the energy code for the resistor under consideration and output terminals (A1, A2) and (C1, C2) are supplied with the energy codes representing the amount of energy supplied to the adjacent resistors. These output codes are supplied to address decoder 34' together with the bit of incoming information to be printed by the corresponding heating resistor. There they are converted to address codes for addressing ROM 36'. ROM 36' stores energy codes which are determined by the input codes A1, A2, B1, B2, C1, C2 and read out at output terminals O1 and O2. The relationship between input codes A1, A2, B1, B2, C1, C2 of address decoder 36' and output code O1, O2 of ROM 36' is shown in the following Truth Table (4).
TRUTH TABLE (4)______________________________________A1 A2 B1 B2 C1 C2 O1 O2 A1 A2 B1 B2 C1 C2 O1 O2______________________________________000 0 0 0 1 1 0 0 1 0 0 0 1 1 010 0 0 0 1 1 0 1 1 0 0 0 1 0 100 0 0 0 1 1 1 0 1 0 0 0 1 0 110 0 0 0 1 1 1 1 1 0 0 0 1 0 010 0 0 1 1 1 0 1 1 0 0 1 1 0 010 0 1 0 1 1 0 1 1 0 1 0 1 0 010 0 1 1 1 1 0 1 1 0 1 1 1 0 100 0 1 0 1 1 1 0 1 0 1 0 1 0 100 0 1 1 1 0 1 0 1 0 1 1 0 1 110 0 1 1 1 0 1 1 1 0 1 1 0 1 000 1 0 0 1 1 0 0 1 1 0 0 1 0 010 1 0 0 1 1 0 1 1 1 0 0 1 0 100 1 0 0 1 1 1 0 1 1 0 0 1 0 110 1 0 0 1 0 1 1 1 1 0 0 0 1 010 1 0 1 1 1 0 1 1 1 0 1 1 0 010 1 1 0 1 0 0 1 1 1 1 0 0 1 010 1 1 1 1 0 0 1 1 1 1 1 0 1 100 1 1 0 1 0 1 0 1 1 1 0 0 1 100 1 1 1 1 0 1 0 1 1 1 1 0 1 110 1 1 1 1 0 1 1 1 1 1 1 0 1______________________________________
This Table, however, only covers the case where G="1". When G is "0", O1 and O2 are determined always to be "0". Again, O1 and O2 take the same value even when the codes A1, A2 and C1, C2 replace each other.
FIGS. 7 and 8 show the way in which the amounts of energy which should be used for heating resistors in the next cycle of printing are determined. In FIG. 7, circles a1, a2 --- of row (a) represent the amounts of energy used in each heating resistor in the previous cycle of printing. Circles b1, b2, - - - of row (b) represent the amounts of energy to be used in each heating resistor in the coming cycle of printing. Letters p1, p2, - - - represent the positions of heating resistors. In FIG. 8 (a)-(d), the circles correspond to different current durations T1 -T3 representing different amounts of energy. As shown in FIG. 7, the amount of energy b3 to be supplied to the resistor at the position p3 in the coming cycle of printing is determined by taking into consideration the amount of energy a2, a3, a4 for the resistors in positions p2, p3, p4 in the previous cycle of printing. Whereas in the previous embodiment b3 would be selected as the longest pulse width or current duration T3, since the amount of electrical energy a3 for the same heating resistor in the previous cycle of printing is 0 (i.e., T=0), in this embodiment, since the amounts of energy a2, a4 (and particularly a4), in the previous cycle of printing were large, the pulse width or current duration is set at T2, a somewhat shorter time than T3. In this way, the output codes (O1, O2) of ROM 36' are stored into RAM 38 as energy codes (N1, N2) to replace the previous ones which should be supplied to each of n heating resistors in the coming cycle of printing. When all the codes (N1, N2) have been written afresh into RAM 38, printing is carried out by thermal head 44 and first control circuit 42 in the same way as has been already explained in relation to the previous embodiment. Further explanation is, therefore, obviated by referring to the corresponding numbers in FIG. 2.
FIGS. 9 to 12 show another embodiment according to the invention in which a facsimile signal is supplied to the thermal printer as incoming picture information. In facsimile equipment using digital transmission in which information is compressed in order to increase transmission speed, transmission time Ta for each line of picture data G is liable to change as shown in FIG. 9(a). This is one of the factors resulting in lack of uniformity in printing. The reason is that for the picture information G in FIG. 9(a), heating resistors of the thermal printer are supplied with current for the periods marked T in FIG. 9(b); but if the transmission time Ta changes, the printing cycle time Tb changes also. Now, as shown in FIG. 10, there is a non-linear relationship between printing cycle time and printing density. When the printing cycle time is longer than a given value Tc, printing density is more or less constant; but if it is shorter than Tc, printing density rises sharply. The reason for this is that, during most of the printing cycle, the heating resistors are cooling off. Only a small fraction of the printing cycle involves supplying current to the resistors. Therefore, the longer the printing cycle, the more time the resistors have to cool and the less dense is the printing, until time Tc is reached. This embodiment has been devised with this point in mind. As shown in FIG. 11, a thermal printer according to this embodiment has a transmission time detection circuit 52 added to the thermal printer system shown in FIG. 2. Incoming facsimile information G is serially input into terminal 32 and supplied to address decoder 34. Information G is also supplied to sync separator 54 which separates, from the picture data, sync signal PRD indicating the position of the start of each line of picture data G. Sync signal PRD is fed to transmission time detection circuit 52, where code P, indicating the transmission time of each line of picture data G, is developed. FIG. 12 shows an example of transmission time detection circuit 52. Sync signal PRD is supplied to a loading terminal 522 of a counter 524 and sets the counter to zero. Decoder 526 provides an output of "0" to an AND gate 528 by providing a "1" to an inverter 530 when counter 524 is set to zero, and opens AND gate 528. Clock pulse CK from second control circuit 46 in FIG. 11 is then supplied to counter 524 via a terminal 527 and AND gate 528. Counter 524 begins to count, and so measures the transmission time of the picture data G. When the contents of counter 524 reach a value corresponding to Tc in FIG. 10, decoder 526 produces an output of "1", and the counter stops. The output of decoder 526 is latched to a latching circuit 532 by the next sync signal PRD. The output signal P of latching circuit 532 is fed from a terminal 533 to address decoder 34 in FIG. 11 together with the energy codes (M1, M2) and picture data G. Consequently, when the transmission time of a particular line of picture data G reaches Tc, P becomes "1"; until then, P is "0". Address decoder 34 supplies its output to ROM 36 to designate an address in ROM 36 and an energy code stored at the designated address is read out at its output (O1, O2) in the same manner as already described above. The relationship between the input codes (M1, M2, G, P) to address decoder 34 and output codes (O1, O2) of ROM 36 is shown in the following Truth Table (5).
TRUTH TABLE (5)______________________________________G P M1 M2 O1 O2______________________________________1 0 0 0 1 11 1 0 0 1 11 0 1 0 0 11 1 1 0 0 11 0 0 1 0 11 1 0 1 0 11 0 1 1 1 01 1 1 1 0 1______________________________________
When G is "0", O1 and O2 are "0". The outputs of ROM 36 are stored in RAM 38 as energy codes (N1, N2) and the same printing process occurs as mentioned above. Further explanation of the embodiment is, therefore, obviated by referring to the corresponding numbers in FIG. 2.
FIG. 13 shows a further embodiment of the thermal printer according to the invention in which the transmission time detecting circuit 52 is added to the thermal printer shown in FIG. 6. In this embodiment, the amount of energy of adjacent heating resistors in the previous printing cycle and the transmission time of picture data for each line are both taken into consideration in determining the amount of energy for each heating resistor in the coming cycle of printing. Address decoder 34" and ROM 36" are so designed that input codes A1, A2, B1, B2, C1, C2, P and data G to address decoder 34" are related to the output code O1, O2 as shown in the following Truth Table (6).
TRUTH TABLE (6)______________________________________P = "1" P = "0"A1 A2 B1 B2 C1 C2 O1 O2 A1 A2 B1 B2 C1 C2 O1 O2______________________________________000 0 0 0 1 1 0 0 0 0 0 0 1 1 010 0 0 0 1 1 0 1 0 0 0 0 1 1 100 0 0 0 1 1 1 0 0 0 0 0 1 1 110 0 0 0 1 1 1 1 0 0 0 0 1 1 010 0 0 1 1 1 0 1 0 0 0 1 1 1 010 0 1 0 1 1 0 1 0 0 1 0 1 1 010 0 1 1 1 1 0 1 0 0 1 1 1 1 100 0 1 0 1 1 1 0 0 0 1 0 1 1 100 0 1 1 1 0 1 0 0 0 1 1 1 1 110 0 1 1 1 0 1 1 0 0 1 1 1 1 000 1 0 0 1 1 0 0 0 1 0 0 1 1 010 1 0 0 1 1 0 1 0 1 0 0 1 1 100 1 0 0 1 1 1 0 0 1 0 0 1 1 110 1 0 0 1 0 1 1 0 1 0 0 1 1 010 1 0 1 1 1 0 1 0 1 0 1 1 1 010 1 1 0 1 0 0 1 0 1 1 0 1 1 010 1 1 1 1 0 0 1 0 1 1 1 1 0 100 1 1 0 1 0 1 0 0 1 1 0 1 0 100 1 1 1 1 0 1 0 0 1 1 1 1 0 110 1 1 1 1 0 1 1 0 1 1 1 1 0 001 0 0 0 1 1 0 0 1 0 0 0 1 1 011 0 0 0 1 0 0 1 1 0 0 0 1 0 101 0 0 0 1 0 1 0 1 0 0 0 1 0 111 0 0 0 1 0 1 1 1 0 0 0 1 0 011 0 0 1 1 0 0 1 1 0 0 1 1 0 011 0 1 0 1 0 0 1 1 0 1 0 1 0 011 0 1 1 1 0 0 1 1 0 1 1 1 0 101 0 1 0 1 0 1 0 1 0 1 0 1 0 101 0 1 1 0 1 1 0 1 0 1 1 1 0 111 0 1 1 0 1 1 1 1 0 1 1 1 0 001 1 0 0 1 0 0 0 1 1 0 0 1 0 011 1 0 0 1 0 0 1 1 1 0 0 1 0 101 1 0 0 1 0 1 0 1 1 0 0 1 0 111 1 0 0 0 1 1 1 1 1 0 0 1 0 011 1 0 1 1 0 0 1 1 1 0 1 1 0 011 1 1 0 0 1 0 1 1 1 1 0 1 0 011 1 1 1 0 1 0 1 1 1 1 1 0 1 101 1 1 0 0 1 1 0 1 1 1 0 0 1 101 1 1 1 0 1 1 0 1 1 1 1 0 1 111 1 1 1 0 1 1 1 1 1 1 1 0 1______________________________________
In FIG. 13, parts are numbered correspondingly to those in FIGS. 6 and 11 and the description accompanying those figures will suffice to explain the embodiment.
It should be noted that there can be many modifications within the scope of the invention. A 2-input multiplexer 72, shown in FIG. 14, can be substituted for decoder 422 and multiplexer 424 in FIG. 4. In this case, one cycle of printing for one line is divided into two subcycle periods (I and II) in each of which energy code (N1, N2) is read out as shown in FIG. 15 and supplied to the inputs of multiplexer 72. Multiplexer 72 is controlled by selection signal S so that in the first subcycle period the code data N1, and in the second subcycle period the code data N2, are selected as its gating signal Y and supplied to input terminal 26 of shift register 22 in FIG. 4. When all the code data N1 for each heating resistor are stored in shift register 22 during subcycle period I, latch pulse LP1 latches the output signals of the shift register for T1 until latch pulse LP2 is applied to the shift register. By this means, selected heating resistors are supplied with current for the time period T1 as shown in FIG. 15. In subcycle period II, code data N2 are stored in shift register 22 and output signals of the shift register 22 are latched during the time period of T2 by latch pulses LP2 and LP3. By this means, selected heating resistors are supplied with current for the time period T2. In this case when the energy codes N1, N2 are both "1" current is supplied during both time periods T1 and T2. The energy code (N1, N2), therefore, can provide three different amounts of energy, T1, T2 and T1 +T2 corresponding to the codes (1, 0), (0, 1) and (1,1), giving the same results as previously. The advantage of this variation is that printing time is reduced, since a single printing cycle lasts only from LP1 to LP3 and not from LP1 to LP4, as before. The different time periods during which energy is supplied to the heating resistors may therefore overlap. For example, time periods T1 and T3 are overlapping time periods. Also, T2 and T3 are overlapping time periods. T1 and T2, however, do not overlap.
Demultiplexer 62 and address decoder 34' in FIG. 6 can be replaced by an address decoder shown in FIG. 16. The decoder includes six flip-flop circuits 821, - - - 826 which are connected in series to form a shift register. Energy codes (M1, M2) in the previous cycle of printing are supplied from RAM 38 to flip-flops 825 and 826 via NAND gates 841 and 842. These NAND gates 841 and 842 are controlled together with another set of NAND gates 861 and 862 by strobe signal STB from second control circuit 46 of FIG. 6, via inverter 88. Strobe signal STB opens NAND gates 841, 842, 861, 862 to write the energy code (M1, M2) into a set of flip-flops 825, 826. Operation of this address decoder is now explained taking as an example a case in which the amount of energy b3 which should be supplied to a heating resistor at the position p3 in FIG. 7 is determined. At first, energy code (M1, M2) representing a2 for the resistor at position p2 in FIG. 7(a) is read out from RAM 38 and written into flip-flops 825 and 826 by strobe signal STB. Then clock signal CK1 from second control circuit 46 in FIG. 6 is supplied to all the flip-flops to shift the code (M1, M2) into flip-flops 823, 824. Second, the energy code (M1, M2) representing a3 for the resistor at position p3 is read out from RAM 38 and written into flip-flops 825, 826 by the next strobe signal STB. Again clock signal CK1 is supplied to shift the codes (M1, M2) stored in flip-flops 823, 824 and 825, 826 to the next pair of flip-flops 821, 822 and 823, 824 in turn. Finally, energy code (M1, M2) representing a4 for the resistor at position p4 is read out from RAM 38 and is written into the pair of flip-flops 825, 826. At this time three sets of energy codes (M1, M2) have been stored in the three pairs of flip-flops. Output signals of each flip-flop A1, A2, B1, B2, C1, C2 and a bit of incoming information G to be printed in the coming cycle of printing by the heating resistor at position p3 are supplied to ROM 36' to address. At the output terminals O1, O2 of ROM 36' the new energy code (O1, O2) is provided representing b3 for the resistor at position p3.
In the embodiments mentioned above, although only one RAM 38 is used, it is also possible to use two RAMs 381, 382 as shown in FIG. 17.
In FIG. 17, energy code M1, M2 is read first from RAM 381 via a selector 1022 and supplied to address decoder 34 (in FIG. 2) or demultiplexer 62 (in FIG. 6) in a given printing cycle. After that, the output code of ROM 36 in FIG. 2 (or 36' in FIG. 6) is written, via selector 1021, into RAM 381 as the energy code (N1, N2). Energy code (N1, N2) is read from another RAM 382 via selector 1022 and supplied to first control circuit 42 in FIGS. 2 or 6. Then, in the next printing cycle, codes (M1, M2) are read from RAM 382, converted by ROM 36 or 36' and rewritten into RAM 382 via selector 1021. Energy code (N1, N2) is read out from RAM 381 and supplied to the first control circuit 42. The two RAMs are therefore used alternately to provide either the energy code for the preceding printing cycle, M1, M2, or the energy code for the next cycle, N1, N2. For example, if the energy code (N1, N2) for the current printing cycle is stored in RAM 381, the next printing cycle's energy code (N1, N2) will be stored in RAM 382. When the next printing cycle arrives, the data stored in RAM 381 is read out as energy codes (M1, M2) for the previous printing cycle and used to determine energy codes (N1, N2) for the present cycle.
It can be seen from the embodiment illustrated in FIG. 17, that determining amounts of electrical energy for the coming cycle of printing based on codes (M1, M2) of the previous cycle, and reading the codes (N1, N2) for the coming cycle, occur simultaneously. This is very suitable for cases when picture data are input in a continuous time series, as in facsimile receiving equipment.
The means of controlling the amount of electrical energy need not be limited to variation of the current duration or pulse width; it is equally possible, for example, to vary the voltage or current applied to the heating resistors.
Shift register 22 shown in FIGS. 1 and 4 can be divided into several groups SR1 -SRk with control terminals 311, 312, - - - 31k controlling the output from each group as shown in FIG. 18. By supplying signals into these terminals 311, 312 - - - 31k in turn, heating resistors can be driven in groups instead of all at once. Further, the shift register 22 can be replaced by an ordinary diode matrix system.
The invention still can be put into practice in various other forms. A shift register can be used instead of the RAM as a means of storing the codes representing amounts of electrical energy.
The data indicating the amount of electrical energy can also be encoded by a number of bits greater than 2.
Although illustrative embodiments of the invention have been described in detail with reference to the accompanying drawings, it is to be understood that the invention is not limited to those precise embodiments and that various changes and modifications may be effected therein by one skilled in the art without departing from the scope or spirit of the invention.
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|Jun 16, 1982||AS||Assignment|
Owner name: TOKYO SHIBAURA DENKI KABUSHIKI KAISHA, 72, HORIKAW
Free format text: ASSIGNMENT OF ASSIGNORS INTEREST.;ASSIGNORS:SEKIYA, KUNIHIKO;MIZUGUCHI, MAMORU;OOZEKI, TAKASHI;REEL/FRAME:004008/0872
Effective date: 19820603
Owner name: TOKYO SHIBAURA DENKI KABUSHIKI KAISHA, A CORP. OF
Free format text: ASSIGNMENT OF ASSIGNORS INTEREST;ASSIGNORS:SEKIYA, KUNIHIKO;MIZUGUCHI, MAMORU;OOZEKI, TAKASHI;REEL/FRAME:004008/0872
Effective date: 19820603
|Jan 26, 1988||FPAY||Fee payment|
Year of fee payment: 4
|Sep 30, 1991||FPAY||Fee payment|
Year of fee payment: 8
|Mar 12, 1996||REMI||Maintenance fee reminder mailed|
|Aug 4, 1996||LAPS||Lapse for failure to pay maintenance fees|
|Oct 15, 1996||FP||Expired due to failure to pay maintenance fee|
Effective date: 19960807